新型稀磁半导体Cd1-xMnxIn2Te4的光学和磁学性能

采用垂直Bridgman法制备出了x＝0.1、0.22和0.4的Cd1-xMnxIn2Te4晶体.采用红外透射光谱法研究了晶体的红外光学特性.用超导量子磁强计测量了样品在温度范围5～300K和磁场强度范围0～5T内的磁化强度.在中红外波段透过率曲线变化很小.随着x的增加Cd1-xMnxIn2Te4的光学带隙移向高能端.磁化率倒数χ-1与温度T的关系曲线在高温区服从居里-万斯定律,在低温下x≥0.22时向下偏离该定律.与具有相同Mn2+浓度的Cd1-xMnxTe晶体相比Cd1-xMnxIn2Te4晶体的交换积分常数较小.     

高阻CdZnTe晶体的退火处理

获得高电阻率的、完整性好的 Cd Zn Te晶体是研制高性能的 Cd Zn Teγ射线探测器的关键 .运用热力学关系估算了 Cd1 - x Znx 熔体平衡分压 ,尝试以 Cd1 - x Znx 合金源替代 Cd源进行 Cd0 .8Zn0 .2 Te晶片的热处理 ,研究了退火对 Cd0 .8Zn0 .2 Te晶片质量的影响 .结果表明 :在 10 6 9K下用 Cd0 .8Zn0 .2 合金源 (PZn=0 .12 2e5 Pa和 PCd=1.2 0e5 Pa)对 Cd0 .8Zn0 .2 Te晶片退火 5天以上 ,可提高晶体电阻率一个数量级和晶体红外透过率 10 %以上 ,并可消除或减小晶片中的 Te沉淀 ,同时避免了 Zn的损失 ,改善 Zn的径向分布 .可见 ,采用 Cd1 - x Zn     

Pb_(1 - x) Ge_x Te薄膜的光学性质

对 PVD沉积 Pb1 - x Gex Te薄膜研究发现 Pb1 - x Gex Te是一种高性能的红外材料 ,在 3～ 2 5μm光谱范围具有较好的透光性能 ,室温下的折射率为 4.8～ 5 .6 .薄膜的光学性质 ,包括透射率、色散关系以及折射率的温度系数dn/ d T,与材料中组分 x、环境温度和薄膜的沉积工艺条件有密切关系 .适当地改变组分和工艺条件 ,可以使薄膜的折射率温度系数 dn/ d T从负变到零并转为正 ,这对于制备高温度稳定性的红外光学薄膜器件具有重要的意义     

资料简介索引

红外器件 2Q01 Hg,一二cd汀e的红外光学吸收 Infrared optieal absorption of Hgl一二Cd言Te, E .Finkman,Israel Institu七e of Teehno土ogy,J Appl.P!1丁5.5 June 1979,Vol 50,No6,pp. 4356一4361. 在80到300K温度下测量了整个0 .205成x蕊0.220组分范围的接近Hgl一二Cd二Te基础吸收边缘的吸收。根据干涉图案得出了Hg,一考C(坛Te折射率的色散。发现吸收尾部服从于改进的urbach法则,并用20落a(厘米一‘)(2000的a=aoexp〔a(百一E。)/(T+T。)〕表示。拟合参数a。,a,T。和E。随x有规则地变化。表示式用于求作为二和T函数的能隙吸收…     

10.6μm激光辐照碲镉汞红外探测器热损伤研究

研究了Hg Cd Te红外探测器的结构以及材料特性,阐述了激光损伤Hg Cd Te红外探测器的机理,建立了Hg Cd Te红外探测器三维仿真模型,利用有限元分析法,对10.6μm CO2激光辐照Hg Cd Te探测器的温度变化情况进行了仿真,并通过参考已有文献的实验数据,验证了模型的准确性。当Hg Cd Te探测器受到峰值功率密度为5×107 W/cm2的单脉冲激光辐照时,Hg Cd Te晶体的Hg离子开始析出,探测器性能降低,并不可恢复;当激光峰值功率为108 W/cm2,探测器Hg Cd Te晶体开始出现熔融现象,此时激光能量密度为1 J/cm2;当激光峰值功率为2×108 W/cm2时,铟柱达到熔融温度,探测器会出现铟柱脱落现象,被彻底损坏。     

Cd_(1-x)Zn_xTe多晶薄膜的制备、性能与光伏应用

用共蒸发法制备了 Cd1 - x Znx Te多晶薄膜 ,薄膜结构属立方晶系空间群 F4 3m.通过透射光谱的测量 ,计算光能隙 ,得到室温时薄膜的光能隙随组分 x值的变化满足二次方关系 .作为对异质结界面的修饰 ,提出了有 Cd1 - x-Znx Te过渡层的 Cd S/ Cd Te/ Cd1 - x Znx Te/ Zn Te∶ Cu电池 .并在相同工艺下制备了 Cd S/ Cd Te/ Cd0 .4 Zn0 .6 Te/ Zn Te∶ Cu与 Cd S/ Cd Te/ Zn Te∶ Cu太阳电池 ,发现前者比后者效率平均增加了 35 .0 % .     

加压布里奇曼法生长大直径HgCdTe晶体

根据加压改进布里奇曼法 ,采用“二次配料”工艺成功地生长了直径 40 mm的大直径 Hg Cd Te (组分 x≈0 .2 0 )晶体 .采用加压技术 ,平衡部分石英安瓶内的高汞蒸汽压 ,有效地避免了石英安瓶的爆裂 ;采用“二次配料”工艺 ,大大降低了生长温度 ;合理选择温度梯度和生长速度 ,获得了有较好结晶性和组分均匀性的 Hg Cd Te晶体 .分析表明 :Hg Cd Te晶片的载流子浓度 n77≤ 4× 10 1 4 cm- 3 ,迁移率 μ77≥ 1× 10 5 cm2 /(V· s) ,少数载流子寿命值 τ≥ 2 .0 μs,80 K时简单的性能测试用光导探测器件的探测率 D*为 1.1× 10 1 0 cm· Hz1 /2 /W.     

高阻值Cd1-xZnxTe晶体的生长及其性能测试

通过适当的工艺措施,采用Bridgman法生长了直径为30mm的X射线及γ射线探测器级的Cd0.9Zn0.1Te晶锭.测试结果表明:该晶锭结晶质量良好,位错密度低,成分均匀,杂质含量低,红外透过率和电阻率都十分接近本征Cd0.9Zn0.1Te的值.并从晶体的生长特性、缺陷和杂质的角度,分析了生长高性能晶体的条件,研究了生长Cd1-xZnxTe晶体的x值与缺陷和杂质浓度之间的关系.     

高阻值Cd_(1-x)Zn_xTe晶体的生长及其性能测试

通过适当的工艺措施,采用Bridgman法生长了直径为30mm的X射线及γ射线探测器级的Cd0 9Zn0 1Te晶锭.测试结果表明:该晶锭结晶质量良好,位错密度低,成分均匀,杂质含量低,红外透过率和电阻率都十分接近本征Cd0 9Zn0 1Te的值.并从晶体的生长特性、缺陷和杂质的角度,分析了生长高性能晶体的条件,研究了生长Cd1-xZnxTe晶体的x值与缺陷和杂质浓度之间的关系     

HgCdTe分子束外延In掺杂研究

报道了用 MBE方法生长掺 In的 n型 Hg Cd Te材料的研究结果 .发现 In作为 n型施主在 Hg Cd Te中电学激活率接近 10 0 % ,其施主电离激活能至少小于 0 .6 m e V.确认了在制备红外焦平面探测器时有必要将掺杂浓度控制在～ 3× 10 1 5 cm- 3水平 .比较了高温退火前后 In在 Hg Cd Te中的扩散行为 ,得出在 40 0℃温度下 In的扩散系数约为10 - 1 4 cm2 / s,并确认了 In原子作为 Hg Cd Te材料的 n型掺杂剂的可用性和有效性 .     

磁性石榴石薄膜的磁力显微镜研究

本文采用磁力显微镜（ＭＦＭ）对磁性石榴石（ＹＧｄＢｉ）３（ＧａＦｅ）５Ｏ１２薄膜的磁畴结构进行了观察研究。实验结果表明，磁性针尖的磁特性进行对石榴石ＭＦＭ图像的影响较大，而且随着针尖与样品间距的增大，磁针尖对石榴石畴结构的影响有所降低。另外，改变针尖的磁化方向，得到的石榴石磁畴结构也有所不同。     

磁感应或磁共振,哪个更适合于无线充电?

磁感应与磁共振是目前最主要的两种无线充电技术,本文分析各种技术的优缺点。本文网络版地址:http://www.eepw.com.cn/article/145521.htm     

Magnetic megabits

Improvements in recording densities that are allowing magnetic storage to pack more data than its optical counterparts are examined. The technologies that have driven the advances are discussed. They consist of highly sensitive magnetoresistive heads, ultra-low-noise magnetic media, and advanced signal detection techniques. Disk and tape performances are compared     

Multiple Magnetic States of Silicon Carbide Diluted Magnetic Semiconductors

Calculations from first principles density functional theory are used to study magnetic properties of silicon carbide doped with several percent of first row transition metal impurities. It is shown that transition-metal-doped SiC can be in either a nonmagnetic or a magnetic state. For different impurities the two states are separated by an energy gap with the width on the order of several tens of milli-electron volts or the transition between the states is gradual. We suggest that, at a high enough temperature, the relationship between the states can change or there can exist a new state which is a mix of the magnetic and nonmagnetic states. Calculated mean-field values of the Curie temperature suggest that ferromagnetic ordering at room temperature is possible in Mn-doped SiC.     

磁场中硅熔体的磁黏度

利用魔环磁场,对硅熔体施加横向可调的磁场.采用回转振荡法,测量了硅熔体在不同温度、不同水平方向磁场下的磁黏度.研究结果表明,引入磁场,使硅熔体的磁黏度增加,且磁黏度与磁场强度呈抛物线关系.     

磁场中硅熔体的磁黏度

利用魔环磁场,对硅熔体施加横向可调的磁场.采用回转振荡法,测量了硅熔体在不同温度、不同水平方向磁场下的磁黏度.研究结果表明,引入磁场,使硅熔体的磁黏度增加,且磁黏度与磁场强度呈抛物线关系.     

Magnetic resonance imaging

Signal processing lies at the core of MRI. Data acquisition and manipulation occur naturally in the spatial Fourier transform domain of the image. A review of the imaging process and the associated image characteristics reveals the many opportunities for contributions from the signal processing community. This article develops the Fourier representation of the imaging process from an overview of the physics of the MRI signal. This article also discusses tradeoffs in acquisition time, resolution, and field of view as well as image degradation associated with noise and motion artifacts. In addition, the ability to manipulate soft tissue contrast over a wide range of independent parameters in MRI is outlined     

FePt Magnetic Nanoparticles and Their Assembly for Future Magnetic Media

Magnetic nanoparticles with extremely high anisotropy such as chemically ordered $hbox{L}1_{0}$ phase FePt nanoparticles have been considered one of the best candidates for future magnetic recording media with areal density beyond 1 ${ hbox{Tbit/in}}^{2}$ for either the nanocomposite-film-type heat-assisted magnetic recording (HAMR) media or the self-organized-magnetic-array (SOMA)-type bit patterned media. However, current preparation methods via phase transformation must overcome many obstacles, including particle agglomeration, twinning, and difficulty of easy axis alignment. In this paper, the effort on and promise of the preparation of monodispersed magnetic nanoparticles with high anisotropy by a gas phase condensation method is reviewed and reported. The focus is to review recent progress on the fabrication of monodispersed highly ordered $ hbox{L}1_{0}$ phase FePt nanoparticles without phase transformation, successfully self-assembled and magnetically aligned magnetic nanoparticles for SOMA and HAMR media. The mechanisms for directly forming $hbox{L}1_{0}$ phase FePt nanoparticles during nucleation and growth processes and magnetically aligning these particles are analyzed.      

Magnetic Field Converters Based on the Spin-Tunnel Magnetic Resistance Effect

Russian Microelectronics - The modern designs of magnetic field transducers (MFTs) based on nanostructures with the spin-tunnel magnetoresistive effect (STMR) and the main areas of their...     

Magnetic recording systems

This review of magnetic recording systems concentrates on developments in two particular areas: the video-tape recorder and the rigid disk drive. The consumer VCR represents the state of the art for analog in-contact recording, while the rigid disk drive exemplifies digital recording with rapid access. Various aspects of the mechanical configurations, track-following techniques, heads and media, and signal processing are discussed. More briefly the paper describes other digital systems on flexible media.